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1.
使用密度泛函理论(DFT)和含时密度泛函理论(TDDFT)以及自然键轨道(NBO)分析,设计比有机染料D5更优秀的用于染料敏化太阳能电池(DSSC)的D5同类物分子.在D5骨架的给电子基团上对称地引入给电子基(—OH,—NH2,—OCH3),既可以使分子的最低未占据分子轨道(LUMO)能级提高,又可以使吸收光谱红移,从而既提高染料分子捕获太阳辐射光子的能力,又提高由染料分子的激发态向TiO2电极注入电子的驱动力.在D5分子的骨架上,对称地引入受电子基(—CF3,—F,—CN),可以使染料分子的吸收光谱强烈地红移,从而更有效地利用太阳能.由LUMO能级的提高和吸收光谱的红移来考虑,所设计的D516,D536,D537分子是比D5优秀的同类物分子,其中D516是最好的.单从吸收光谱红移来考虑,所设计的D565,D567,D568分子是比D5优秀的同类物分子,其中D565的吸收光谱有望与太阳辐射光谱更好地匹配.挑选出来的这6种D5同类物分子都是D-π-A(电子给体-共轭π桥-电子受体)结构.这几种分子的光激发引起的最高占据分子轨道(HOMOs)到LUMOs的跃迁是π-π*跃迁,是分子内电荷转移,吸收光谱是电子吸收光谱,位于近紫外-可见光区.D516和D565有望成为比D5更优秀的用于DSSC的非金属有机染料分子.  相似文献   

2.
为了揭示D-SS和D-ST分子敏化的染料敏化太阳能电池(DSSCs)的物理机制,采用密度泛函理论(DFT)、含时密度泛函理论(TDDFT)和自然键轨道(NBO)分析,模拟计算染料D-SS和D-ST分子的结构、紫外-可见吸收光谱和能级结构.D-SS的紫外-可见吸收光谱相比于D-ST的有明显的红移,而且D-SS分子的摩尔吸光系数也高于D-ST分子的.D-SS分子本应该比D-ST分子拥有更高的俘获太阳辐射光子的能力,但由于D-SS分子的最高占据分子轨道(HOMO)能级位置比氧化还原电解质(|-/|-3)的氧化还原能级高,处于光激发态的D-SS分子向TiO2电极注入电子而被氧化后,不能顺利地从电解质中得到电子而还原,使得D-SS分子俘获光子的能力不能充分发挥,从而严重地降低了由其敏化的DSSCs的光电性能和光电能量转换效率.揭示了D-SS敏化的DSSCs的光电性能,特别是光电能量转换效率比D-ST敏化的DSSCs的低的原因.染料敏化剂分子的HOMO能级的位置对于DSSCs来说也是很重要的,用于DSSCs的有机敏化剂分子的HOMO能级的位置必须低于氧化还原电解质的氧化还原能级.  相似文献   

3.
采用密度泛函理论和含时密度泛函理论方法计算了2个吩噻嗪类染料及其吸附到TiO2上后分子的基态和激发态光物理性质与热力学参数.结果表明,电子给体的改变虽未明显改变染料的光谱性质(垂直跃迁能和振子强度),但可以改变分子的前线轨道能级,进而影响染料分子的激子结合能Eb及激发态电子注入到半导体TiO2中的驱动力△Gint的大小...  相似文献   

4.
利用密度泛函理论(DFT)和含时密度泛函理论(TD-DFT), 分别基于B3LYP和PBE1PBE方法研究了一系列含有不同给电子基团的吲哚染料分子(ID1-ID3)的电子结构和吸收光谱性质. 重点比较了不同电子给体对染料的分子结构、吸收光谱以及其在电池中的光伏性能的影响. 结果表明从ID1、ID2到ID3, 随着电子给体中苯环数目的增加, 吲哚分子上的共轭效应逐渐增大, 导致吲哚分子最高占据分子轨道-最低未占据分子轨道(HOMO-LUMO)之间的能隙变窄, 分子的吸收光谱发生红移. 染料分子的吸收光谱和LUMO能级分别影响染料的吸光效率和光电转化过程中电子的注入过程, 从而使其二者成为决定电池光伏性能的重要参数. 综合考虑上述两个参数对电池性能的贡献, 通过理论研究证实, 在ID1-ID3系列染料中, ID3具有较长的吸收谱带、较大的分子消光系数和合适的LUMO能级, 从而表现出最为优越的光伏性能, 这与实验得出的结论很好地吻合.  相似文献   

5.
用光电化学方法研究了不对称菁类染料敏化TiO2纳米结构电极的光电转换过程.结果表明,该染料的电子激发态能级位置与TiO2纳米粒子导带边位置匹配较好,光激发染料后,其激发态电子可以注入到TiO2纳米多孔膜的导带,从而使TiO2纳米结构电极的吸收光谱和光电流谱红移至可见光区,其 IPCE(Incident photon-to-electron conversion efficiency)值最高可达84.3%.并进一步结合现场紫外-可见吸收光谱研究了外加电势对激发态染料往TiO2纳米多孔膜注入电子过程的影响.  相似文献   

6.
以染料分子D5为原型, 采用不同类型和数量的共轭桥单元来设计D-π-A 型有机分子. 采用密度泛函理论(DFT)和含时密度泛函理论(TDDFT)来模拟计算分子的形貌、分子轨道能级以及紫外-可见光谱, 为染料敏化太阳能电池(DSSCs)的敏化分子寻找适合的共轭桥. 采用“次甲基链”、“呋喃环”或“噻吩环”、“次甲基链和呋喃环”或“次甲基链和噻吩环”作为共轭桥单元, 使得分子的吸收光谱依次红移. 随着共轭桥单元的增加, 分子的吸收光谱有剧烈的红移, 但随着共轭桥单元数量的进一步增加, 分子吸收光谱的红移现象减弱. 分子的最低未占据分子轨道(LUMO)能级逐渐降低, 而最高占据分子轨道(HOMO)能级逐渐升高. 采用3个“次甲基链和呋喃环”或者“次甲基链和噻吩环”作为共轭桥时, HOMO能级已经高于氧化还原电解质的能级, 而在极性溶液中, 由2个“次甲基链和噻吩环”单元作为有机分子的共轭桥时, 分子的HOMO能级已经高于氧化还原电解质的能级了. 采用“次甲基链和呋喃环”或“次甲基链和噻吩环”单元作为有机分子的共轭桥时, 吸收光谱有明显的红移,但对于DSSCs的敏化分子, 这样的共轭桥单元只能有1-2个, 不宜过多.  相似文献   

7.
崔宏吉  张宪玺  刘颖  郑锋  张修堂 《化学学报》2008,66(18):2043-2051
采用溶剂场极化连续模型在密度泛函B3LYP/6-31G (D)水平上研究了氢卟啉和镁卟啉分子在四氢呋喃(THF)、二甲基亚砜(DMSO)、二氯甲烷(CH2Cl2)、氯仿(CHCl3)这四种不同极性的溶剂环境中的几何结构和分子轨道能级, 从而研究了溶剂效应引起的分子几何构型和轨道能级的变化. 然后采用上述溶剂环境下优化的几何结构在含时密度泛函水平上计算了它们的激发能、吸收波长、跃迁组成和振荡强度. 理论计算结果表明, 对比真空条件下的氢卟啉和镁卟啉分子的几何结构, 溶剂场中两种卟啉分子的几何结构都发生了微弱的变化, 这种变化随溶剂介电常数的增大而有所增强. 计算结果表明溶剂环境中氢卟啉和镁卟啉分子的电子吸收光谱发生了普遍的红移, 结合分子轨道理论对这种变化给出了可能的解释. 在此基础上, 对这种包含溶剂效应的理论分析方法用于检验卟啉类化合物作为染料敏化太阳能电池光敏剂的可行性作了进一步的探讨.  相似文献   

8.
应用密度泛函理论(DFT)方法计算[6,6]-苯基-C61-丁酸甲酯(PCBM)及其苯环对位取代得到的4种衍生物的几何和电子结构. 采用第一激发能校正了分子的最低未占据分子轨道(LUMO)能级, 探讨了推/拉电子基团对分子前线轨道的影响. 在全优化几何构型的基础上, 采用含时密度泛函理论(TD-DFT)方法研究了电子吸收光谱特征和电荷转移态性质, 并讨论了推/拉电子基团对体系电子吸收光谱性质的影响. 通过对重组能和电子亲和势的计算, 预测了PCBM与4种衍生物的电子能力及电子迁移率大小的关系. 结果表明, 在PCBM中, 在苯环的对位引入推电子基团可以提高分子的前线轨道能级, 改变前线轨道电子云分布, 明显增强可见光范围内的吸收强度, 增加可见光范围内的电荷转移吸收, 且激发态的电荷转移随着引入基团推电子能力的增加而增强. 化合物5的激发态分子内电荷转移性质最强, 且具有较独特的光伏性质. 而在同样位置引入拉电子基团, 则降低了分子前线轨道能级对电子吸收光谱的影响.  相似文献   

9.
运用密度泛函理论中的杂化泛函B3LYP研究了高效太阳能电池新型染料敏化剂JK16和JK17的几何结构、电子结构、极化率和超极化率, 并用含时密度泛函理论(TDDFT)研究了电子吸收谱. 基于含时密度泛函理论计算结果和实验结果的定性符合, 指认了在可见和近紫外区的吸收属于π→π*跃迁. 计算结果还表明JK16和JK17激发能最低的三个跃迁都与光诱导电荷转移过程有关, 而且二-二甲基芴氨基苯并噻吩基团对光电转换过程的敏化起主要作用, 发生于染料敏化剂JK16、JK17和TiO2界面之间的电荷转移是由染料分子激发态向半导体导带的电子注入过程. 此外, 通过对JK16和JK17的比较, 分析了亚乙烯基对几何结构、电子结构和谱学特性的影响.  相似文献   

10.
为了研究四硫富瓦烯(TTF)基团对有机染料敏化剂光电性能的影响,以咔唑染料Dye 1为原型,引入TTF基团作为电子给体,设计了咔唑染料Dye 2.采用密度泛函理论(DFT)和含时密度泛函理论(TD-DFT)分别计算模拟了纯染料分子和吸附团簇(TiO2)9后的形貌、分子轨道能级以及紫外-可见吸收光谱,采用周期性密度泛函理论计算模拟染料分子在二氧化钛(101)面吸附的表面形貌.结果发现:在有机染料中引入TTF基团有助于有机染料敏化剂在二氧化钛表面的抗团聚作用和分子内的电荷转移;最为重要的是,TTF基团的强给电子能力极大地增强了有机染料敏化剂的光捕获能力.所有的计算结果表明,TTF基团是一种非常有潜力改善染料敏化剂光电性能的给电子基团.  相似文献   

11.
We now report metal-free organic dyes having a new type of indoline structure, which exhibits high efficiencies in dye-sensitized solar cells. The solar energy to current conversion efficiencies with the new indoline dye was 6.51%. Under the same conditions, the N3 dye was 7.89% and the N719 dye was 8.26%. The new indoline dye was optimized for the amount of 4-tert-butyl pyridine in the electrolyte and cholic acid as a coadsorbent. Subsequently, the solar energy to current conversion efficiencies reached 8.00%. This value was the highest obtained efficiency for dye-sensitized solar cells based on metal-free organic dyes without an antireflection layer.  相似文献   

12.
用密度泛函理论和DMol3程序包对锐钛矿型TiO2(101)表面复合三(8-羟基喹啉-5-羧酸)铁的敏化机理进行了研究. 计算结果表明, 该染料敏化剂经式结构的HOMO(最高占据分子轨道)-LUMO(最低未占据分子轨道)能隙非常小, 很容易受到激发; TiO2纳米晶吸附染料后, HOMO、LUMO 和费米能级都升高, 导致吸附染料后开路电压VOC升高. 并进一步探讨了三(8-羟基喹啉-5-羧酸)铁在TiO2(101)表面复合过程及作用机理.  相似文献   

13.
Metal-free indoline dyes for dye-sensitized solar cells were studied by employing quantum chemistry methods.Comparative study of the properties of both ground and excited states of metal-free indoline dyes for dye-sensitized solar cells revealed: (i) as the number of rhodanine rings increases, the energy di?erence betweenHOMO and LUMO decreases and there is a red shift in the absorption spectrum with the binding energyincreased, and the transition dipole moment decreased; (ii) Based on an analysis of charge di?erential density,we observed that the charge and energy are transfered from the phenylethenyl to the indoline and rhodaninerings; (iii) The electron-hole coherences are mainly on the indoline and rhodanine rings, and the exciton sizesare 30 and 40 atoms for indoline dyes with one and two rhodanline rings, respectively. These results serveas a good example of computer-aided design in metal-free indoline dyes for dye-sensitized solar cells.  相似文献   

14.
Based on spiro[fluorene-9,90-xanthene](SFX, dye 1), the Lindqvist-type polyoxometalate(POM) functionalized with SFX and its derivatives(dyes 2-4) used in dye-sensitized solar cells(DSSCs) were designed and investigated with the density functional theory(DFT) and time-dependent DFT(TD-DFT) calculations. The results indicate that Lindqvist-type POM is the main contribution to the lowest unoccupied molecular orbital(LUMO) and affects the LUMO energies of dyes 2-4. The maximum absorptions of the designed dyes containing POM(dyes 2-4) are red shifted comparing with that of dye 1. The introduction of electron-donating group onto SFX segment is helpful to red shift the absorption spectra. The major factors affecting the performance of DSSCs, including light harvesting and electron injection were evaluated. Considering the absorption spectra and photovoltaic parameters, dyes 3 and 4 are promising high performance dye sensitizers in n-type DSSCs.  相似文献   

15.
A series of novel metal-free organic dyes TC301-TC310 with relatively high HOMO levels were synthesized and applied in dye-sensitized solar cells (DSCs) based on electrolytes that contain Br(-)/Br(3)(-) and I(-)/I(3)(-). The effects of additive Li(+) ions and the HOMO levels of the dyes have an important influence on properties of the dyes and performance of DSCs. The addition of Li(+) ions in electrolytes can broaden the absorption spectra of the dyes on TiO(2) films and shift both the LUMO levels of the dyes and the conduction band of TiO(2), thus leading to the increase of J(sc) and the decrease of V(oc). Upon using Br(-)/Br(3)(-) instead of I(-)/I(3)(-), a large increase of V(oc) is attributed to the enlarged energy difference between the redox potentials of electrolyte and the Fermi level of TiO(2), as well as the suppressed electron recombination. Incident photon to current efficiency (IPCE) action spectra, electrochemical impedance spectra, and nanosecond laser transient absorption reveal that both the electron collection yields and the dye regeneration yields (Φ(r)) depend on the potential difference (the driving forces) between the oxidized dyes and the Br(-)/Br(3)(-) redox couple. For the dyes for which the HOMO levels are more positive than the redox potential of Br(-)/Br(3)(-) sufficient driving forces lead to the longer effective electron-diffusion lengths and almost the same efficient dye regenerations, whereas for the dyes for which the HOMO levels are similar to the redox potential of Br(-)/Br(3)(-), insufficient driving forces lead to shorter effective electron-diffusion lengths and inefficient dye regenerations.  相似文献   

16.
A series of dye molecules was designed theoretically. Particularly, azoles and their derivatives were chosen as the modifying groups linking to ancillary ligands of [Ru(dcbpyH2)2(NCS)2](N3, dcbpy=4,4′-dicarboxy- 2,2′-bipyridine; NCS=thiocyanato). Density functional theory(DFT) based approaches were applied to exploring the electronic structures and properties of all these systems. The dye molecule with 1,2,4-triazole groups which exhibits a very high intensity of absorption in visible region, was obtained. Time-dependent DFT(TD-DFT) results indicate that the ancillary ligand dominates the molecular orbital(MO) energy levels and masters the absorption transition nature to a certain extent. The deprotonation of anchoring ligand not only affects the frontier MO energy levels but also controls the energy gaps of the highest occupied MO(HOMO) to the lowest unoccupied MO(LUMO) and LUMO to LUMO+1 orbital. If the gap between LUMO-LUMO+1 is small enough, the higher efficiency of dye-sensitized solar cell(DSSC) should be expected.  相似文献   

17.
We found that Br-/Br3- is more suitable than an I-/I3- couple in dye-sensitized solar cells in terms of higher open-circuit photovoltage (Voc) production and higher overall energy conversion efficiency (eta) if the dye sensitizer has a more positive potential than that of Br-/Br3-. Under simulated AM1.5 one sun, an eosin Y dye-sensitized solar cell containing 0.4 M LiBr + 0.04 M Br2 electrolyte in acetonitrile yielded a short-circuit photocurrent (Jsc) of 4.63 mA cm(-2), Voc of 0.813 V, and fill factor (FF) of 0.693, corresponding to 2.61% of eta. Under the same conditions except for the electrolyte 0.4 M LiI + 0.04 M I2 in acetonitrile instead, the device produced 1.67% of eta (Jsc = 5.15 mA cm(-2), Voc = 0.451 V, FF = 0.721). Replacement of I-/I3- with Br-/Br3- in eosin Y dye-sensitized solar cells yielded a significant increase in Voc offset by slight decreases in Jsc and FF, leading to an increase in eta by 56%. The significant gain in Voc was attributed to the enlarged energy level difference between the redox potential of the electrolyte and the Fermi level of TiO2 and the suppressed charge recombination as well. The rate for charge recombination between bromine and the injected electrons was determined to be first order in bromine.  相似文献   

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